Course: EE 8741 Power Electronics in
Power Systems
Term: Spring 2002
Prepared
by: Hans Øverseth Røstøen
HVDC
TRANSMISSION, A ECONOMIC CHOICE.
VOLTAGE
DEPENDENT CURRENT ORDER LIMIT (VDCOL)
Electric power transmission was originally
developed with direct current. The availability of transformers and the
development and improvement of induction motors at the beginning of the 20th Century, led to greater appeal and
use of ac transmission.
Power transmission using HVDC lines is more
cost effective than with AC lines, but requires more complicated and expensive
interconnections (converters) at each end of the line. The application of HVDC
power transmission is therefore limited to transmission of large energies over
long distances. Moreover, HVDC is the only practical option when transporting
electric energy through cables over long distances. Another special application
of HVDC is as a link between AC networks of different frequencies, or between
AC networks that become unstable when tied togethter directly. The HVDC link is
here short and the term "back-to-back" is used to characterize such a
configuration.
Dc transmission became practical when long
distances were to be covered or where cables were required. Originally, mercury arc valves were
used in the converters. Thyristors were applied in the late 1960’s and solid
state valves became a reality. In 1969, a contract for the Eel River dc link in
Canada was awarded as the first application of solid state valves for HVDC
transmission.
Today, the highest functional d.c. voltage for
dc transmission is +/- 600 kV for the 785 km transmission line of the Itaipu
scheme in Brazil. Dc transmission is now an integral part of the delivery of
electricity in many countries throughout the world.
The level of losses is designed into a
transmission system and is regulated by the size of conductor selected. Dc and
ac conductors, either as overhead transmission lines or submarine cables can
have lower losses but at higher expense since the larger cross-sectional area
will generally result in lower losses but cost more. When converters are used
for dc transmission in preference to ac transmission, it is generally by
economic choice driven by one of the following reasons:
The HVDC power converter may be
non-controllable if constructed from one or more power diodes in series or
controllable if constructed from one or more thyristors in series. The standard
bridge or converter connection is defined as a double-way connection comprising
six valves or valve arms (six pulse) that are connected as illustrated below.
When electric power flows into the dc valve group from the ac system then it is
considered a rectifier. If power flows from the dc valvegroup into the ac
system, it is an inverter. Each valve consists of many series connected
thyristors in thyristor modules.

Figure 1: Electric circuit configuration of
the basic six pulse valve group with its converter transformer in star-star
connection.
Nearly
all HVDC power converters with thyristor valves are assembled in a converter
bridge of twelve pulse configuration. The most common twelve pulse
configuration is the use of two three phase converter transformers with one dc
side winding as an ungrounded star connection and the other a delta
configuration. Consequently the ac voltages applied to each six pulse valve
group which make up the twelve pulse valve group have a phase difference of 30
degrees which is utilized to cancel the ac side 5th and 7th harmonic currents and dc side 6th harmonic voltage, thus resulting in a significant saving in harmonic
filters. Since the voltage rating of thyristors is several kV, a 500 kV system
may have hundreds of individual thyristors connected in series.

Figure 2: Twelve pulse valve group
configuration with two converter transformers. One transformer in star-star
connection and the other transformer in star-delta connection.
The
central equipment of a dc substation is the thyristor converter and converter
transformer. They may be configured into poles and bipoles. Some dc cable
systems only have one pole or “monopole” configuration and may either use the
ground as a return path when permitted or use an additional cable to avoid
earth currents. Harmonic filters are required on the ac side and usually on the
dc side. The characteristic ac side current harmonics generated by 6 pulse
converters are 6n +/- 1 and 12n +/- 1 for 12 pulse converters where n equals
all positive integers. Ac filters are typically tuned to 11th, 13th, 23rd and 25th harmonics for 12 pulse converters. Tuning to
the 5th
and 7th harmonics is required if the converters
can be configured into 6 pulse operation. Ac side harmonic filters may be
switched with circuit breakers or circuit switches to accommodate reactive
power requirement strategies since these filters generate reactive power at
fundamental frequency. A parallel resonance is naturally created between the
capacitance of the ac filters and the inductive impedance of the ac system. For
the special case where such a resonance is lightly damped and tuned to a
frequency between the 2nd and 4th harmonic, then
a low order harmonic filter at the 2nd or 3rd harmonic may
be required, even for 12 pulse converter operation.

Figure 3: Monopolar and bipolar
configuration.
Characteristic
dc side voltage harmonics generated by a 6 pulse converter are of the order 6n
and when generated by a 12 pulse converter, are of the order 12n. Dc side
filters reduce harmonic current flow on dc transmission lines to minimize
coupling and interference to adjacent voice frequency communication circuits. Where
there is no dc line such as in the back-to-back configuration, dc side filters
may not be required.

Figure 4: Layout of an HVDC substation
Dc
reactors are usually included in each pole of a converter station. They assist
the dc filters in filtering harmonic currents and smooth the dc side current so
that a discontinuous current mode is not reached at low load current operation.
Because rate of change of dc side current is limited by the dc reactor, the
commutation process of the dc converter is made more robust. Surge arresters
across each valve in the converter bridge, across each converter bridge and in
the dc and ac switchyard are coordinated to protect the equipment from all
overvoltages regardless of their source. They may be used in non-standard
applications such as filter protection. Modern HVDC substations use metal-oxide
arresters and their rating and selection is made with careful insulation
coordination design.
Rectification
or inversion for HVDC converters is accomplished through a process known as
line or natural commutation. The valves act as switches so that the ac voltage
is sequentially switched to always provide a dc voltage. With line commutation,
the ac voltage at both the rectifier and inverter must be provided by the ac
networks at each end and should be three phase and relatively free of
harmonics. As each valve switches on, it will begin to conduct current while
the current begins to fall to zero in the next valve to turn off. Commutation
is the process of transfer of current between any two converter valves with
both valves carrying current simultaneously during this process.
Consider
the rectification process. Each valve will switch on when it receives a firing
pulse to its gate and its forward bias voltage becomes more positive than the
forward bias voltage of the conducting valve. The current flow through a
conducting valve does not change instantaneously as it commutates to another
valve because the transfer is through transformer windings. The leakage
reactance of the transformer windings is also the commutation reactance so long
as the ac filters are located on the primary or ac side of the converter
transformer. The commutation reactance at the rectifier and inverter is shown
as an equivalent reactance XC in the figure below. The sum of all the valve currents transferred the
dc side and through the dc reactor is the direct current and it is relatively
flat because of the inductance of the dc reactor.

Figure 5: AC voltage and current waveshapes
associated with dc converter bridges.
At the
inverter, the three phase ac voltage supplied by the ac system provides the
forward and reverse bias conditions of each valve in the converter bridge to
allow commutation of current between valves the same as in the rectifier. The
inverter valve can only turn on and conduct when the positive direct voltage
from the dc line is greater than the back negative voltage derived from the ac
commutation voltage of the ac system at the inverter.
Reversal
of power flow in a line commutated dc link is not possible by reversing the
direction of the direct current. The valves will allow conduction in one
direction only. Power flow can only be reversed in line commutated dc converter
bridges by changing the polarity of the direct voltage. The dual operation of
the converter bridges as either a rectifier or inverter is achieved through
firing control of the grid pulses.
These
converter bridge angles are measured on the three phase valve side voltages and
are based upon steady state conditions with a harmonic free and idealized three
phase commutation voltage. They apply to both inverters and rectifiers.
Delay
angle a. The time expressed in electrical angular measure
from the zero crossing of the idealized sinusoidal commutating voltage to the
starting instant of forward current conduction. If the angel is less than 90
degrees, the converter bridge is a rectifier and if greater than 90 degrees, it
is an inverter.
Advance
angle b. The time expressed in electrical
angular measure from the starting instant of forward current conduction to the
next zero crossing of the idealized sinusoidal commutating voltage. The angle
of advance b is related in degrees to the angle of delay a.
b=180-a
Overlap
angle m. The duration of commutation between
two converter valve arms expressed in electrical angular measure.
Extinction
angle g. The time expressed in electrical
angular measure from the end of current conduction to the next zero crossing of
the idealized sinusoidal commutating voltage. g depends on the angle of advance b and the angle of overlap m.
g=b-m
HVDC
transmission systems must transport very large amounts of electric power that
can only be accomplished under tightly controlled conditions. Dc current and
voltage is precisely controlled to affect the desired power transfer. It is
necessary therefore to continuously and precisely measure system quantities
that include at each converter bridge, the dc current, its dc side voltage and
the delay angle a or for an inverter, its extinction angle g. Two terminal HVDC transmission systems are
the more usual and they have in common a preferred mode of control during
normal operation. Under steady state conditions, the inverter is assigned the
task of controlling the dc voltage. This it may do by maintaining a constant
extinction angle g causing the dc voltage Ud to droop with increasing dc current
Id as shown in the minimum constant
extinction angle g characteristic A-B-C-D. Weaker the ac system is
at the inverter; steeper is the droop in Ud. Alternatively, the
inverter may normally operate in a dc voltage-controlling mode that is the
constant Ud characteristic
B-H-E. This means that the extinction angle g must increase beyond its minimum.

Figure 6: Steady state Ud-Id characteristics
for a two terminal HVDC system.
If the
inverter is operating in a minimum constant g or constant Ud characteristic, the rectifier must
control the dc current Id. The steady state constant current characteristic of the rectifier is
the vertical section Q-C-H-R. Where the rectifier and inverter characteristic
intersect, either at points C or H, is the operating point of the HVDC system.
The
operating point can be reached by action of the on-line tap changers of the
converter transformers. The inverter must establish the dc voltage Ud by adjusting its on-line tap changer
to achieve the desired operating level if it is in constant minimum g control. If in constant Ud control, the on-line tap changer must adjust its tap to allow the
controlled level of Ud be achieved with an extinction angle equal to or slightly larger than
its minimum setting of 18O in this case.
The
on-line tap changers on the converter transformers of the rectifier can be
controlled to adjust their tap settings so that the delay angle a has a working range at a level between approximately 10Oand 15Ofor maintaining the constant current
setting Iorder. If
the inverter is operating in constant dc voltage control at the operating point
H, and if the dc current order Iorder is increased so that the operating point H
moves towards and beyond point B, the inverter mode of control will revert to
constant extinction angle g control and operate on characteristic A-B. Dc
voltage Ud will be less
than the desired value, and so the converter transformer on-line tap changer at
the inverter will boost its dc side voltage until dc voltage control is
resumed.
Not all
HVDC transmission system controls have a constant dc voltage control such as is
depicted by the horizontal characteristic B-H-E. Instead, the constant
extinction angle g control of characteristic A-B-C-D and the tap
changer will provide the dc voltage control.

Figure 7: Rectifier control loop.

Figure 8: Inverter control loop.
The d.c.
current order Iorder is sent to
both the rectifier and inverter. It is usual to subtract a small value of
current order from the Iorder sent to the inverter. This is known as the current margin Imargin. The inverter also has a current
controller and it attempts to control the dc current Id to the value Iorder - Imargin but the current controller at the rectifier normally overrides it to
maintain the dc current at Iorder. This discrepancy is resolved at the inverter in normal steady state operation
as its current controller is not able to keep the dc current to the desired
value of Iorder - Imargin and is forced out of action. The
current control at the inverter becomes active only when the current control at
the rectifier ceases when its delay angle a is pegged against its minimum delay
angle limit. This is readily observed in the operating characteristics where
the minimum delay angle limit at the rectifier is characteristic P-Q. If for
some reason or other such as a low ac commutating voltage at the rectifier end,
the P-Q characteristic falls below points or E, the operating point will shift
from point H to somewhere on the vertical characteristic D-E-F where it is
intersected by the lowered P-Q characteristic. The inverter reverts to current
control, controlling the dc current Id to the value Iorder - Imargin and the rectifier is effectively
controlling dc voltage so long as it is operating at its minimum delay angle
characteristic P-Q. The controls can be designed such that the transition from
the rectifier controlling current to the inverter controlling current is
automatic and smooth.

Figure 9: Dc current controller at an
inverter.
During
disturbances where the ac voltage at the rectifier or inverter is depressed, it
will not be helpful to a weak ac system if the HVDC transmission system
attempts to maintain full load current. A sag in ac voltage at either end will
result in a lowered dc voltage too. The dc control characteristics shown above
indicates the dc current order is reduced if the
dc
voltage is lowered. This can be observed in the rectifier characteristic R-S-T
and in the inverter characteristic F-G. The controller that reduces the maximum
current order is known as a voltage dependent current order limit or VDCOL
(sometimes referred to as a VDCL).
The VDCOL
control, if invoked by an ac system disturbance will keep the dc current Id to the lowered limit during recovery
which aids the corresponding recovery of the dc system. Only when dc voltage Ud has recovered sufficiently will the
dc current return to its original Iorder
level.

Figure 10: Modifying the current order with a
voltage dependent current order control.
There are
a number of special purpose controllers that can be added to HVDC controls to
take advantage of the fast response of a dc link and help the performance of
the ac system. These include:
Ac
system damping controls. An ac. system is subject to power swings due to electromechanical
oscillations. A controller can be added to modulate the dc power order or dc
current order to add damping. The frequency or voltage phase angle of the ac
system is measured at one or both ends of the dc link, and the controller is
designed to adjust the power of the dc link accordingly.
Ac
system frequency control. A slow responding controller can also adjust the power of the dc link
to help regulate power system frequency. If the rectifier and inverter are in
asynchronous power systems, the dc controller can draw power from one system to
the other to assist in frequency stabilization of each.
Step
change power adjustment. A non-continuous power adjustment can be implemented to take advantage
of the ability of a HVDC transmission system to rapidly reduce or increase
power. If ac system protection determines that a generator or ac transmission
line is to be tripped, a signal can be sent to the dc controls to change its
power or current order by an amount that will compensate the loss. This feature
is useful in helping maintain ac system stability and to ease the shock of a
disturbance over a wider area.
Ac
undervoltage compensation. Some portions of an electric power system are prone to ac voltage
collapse. If a HVDC transmission system is in such an area, a control can be
implemented which on detecting the ac voltage drop and the rate at which it is
dropping, a fast power or current order reduction of the dc link can be
affected. The reduction in power and reactive power can remove the undervoltage
stress on the ac system and restore its voltage to normal.
Subsynchronous
oscillation damping.
A steam turbine and electric generator can have mechanical subsynchronous
oscillation modes between the various turbine stages and the generator. If such
a generator feeds into the rectifier of a dc link, supplementary control may be
required on the dc link to ensure the subsynchronous oscillation modes of concern are positively
damped to limit torsional stresses on the turbine shaft.
Power
systems are steadily growing with ever-larger capacity. Formerly separated
systems are interconnected to each other. Modern power systems have evolved
into systems of very large size, stretching out hundreds and thousands of
kilometers. With growing generation capacity, different areas in a power system
are added with ever-larger inertia.
Furthermore
the unbundling of generation, transmission and supply is less oriented towards
the physical nature of the synchronously interconnected power systems, which
span a large area with interaction among the different sub networks and the
power plants. However in the new environment with possible higher loading of
the transmission system the network operators may be forced to operate the
system closer to its stability limits.
As a
consequence in large interconnected power systems small signal stability,
especially inter-area oscillations, become an increasing importance. Inter-area
oscillation is a common problem in large power systems world-wide. Many
electric systems world-wide are experiencing increased loading on portions of
their transmission systems, which can, and sometimes do, lead to poorly damped
inter-area oscillations. This topic is treated intensively for a long time for
those power systems, where the extension of the interconnected systems and/or
high transmission load led to stability problems.
High-voltage
direct current (HVDC) transmission systems offer a powerful alternative to
increase the stability of a power system as well as to improve system operating
flexibility. The application of HVDC technology is of special interest to
transfer massive amounts of remote hydroelectric power over large distances. In
complex interconnected systems, however, the application of this technology to
achieve the most effective stabilization of critical inter-area modes requires
proper assessment of many interacting factors such as the location of the DC
link, the control configuration and the use of modulation controls.
From
earlier studies it became apparent that with appropriate control, a DC line
could be made to respond more quickly to demands for power flow than could an
AC line. Disturbances such as 3-phase faults, sudden load changes, and sudden
changes in DC reference current setting were investigated.
Methods
of stabilizing an AC system by utilizing a parallel DC line are proposed.
Idealized 2-machine system with parallel AC and DC links are considered to
establish and evaluate several methods of control, which may be used to improve
system stability.
For the
case of 1-machine, infinite bus AC-DC system the change in AC power transmitted
may be expressed:
, where:
E1, E2 – buses
voltages,
- initial angle
between bus voltages,
- change in speed
of the synchronous machine,
- the operator
d/dt.
Change in
rotor speed due to a small change in accelerating power nay be written:
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where H
is inertia constant of the machine.
Either a
current or a power regulator can control the DC power. Incorporated with this
control is a signal dependent upon the change in speed of the machine. Thus,
variation from a constant DC power will be determined by a function of Dw, that is:
=![]()
).
Making a
small change in system power
the change in the
rating power can be expressed:
![]()
and,
using above equations we can express
as:
.
It is
apparent that system damping can be achieved by making
directly proportional
to
. Moreover,
can be selected so as
to define the steady-state operation after a change in Pt has occurred. The
change in system power is accepted by the AC system. More important, however,
is the fact that with
, system damping can be controlled by rating K0. Thus a
change in power might be accepted altering the AC transmitted power in a
critically damped manner. Since the incorporation of a signal promptly
proportional to the change in rotor speed process system damping, it seems
logical to include this signal as a part of any proposed
.
Steady-state
operation is influenced if:
.
It is
apparent that the value of K1 determines the steady-state mode of operation
after a change in system power. If, for example, K1 is made large so that
<<1
![]()
.
Also,
with this type of control, the deviation in the phase angle between bus
voltages may be limited during a break in the link (E1E2/X=0) providing the DC
system is capable of sustaining the necessary overload.
The phase
angle between the bus voltages will return to its value prior to a system
disturbance with:
.
Three
basic methods of control can be determined:
Type A ![]()
Type B ![]()
Type C ![]()
In our
investigation we use method Type B.
A simple system is simulated. The system is
shown in Figure
11.

Figure 11Simple HVDC circuit model.
A load is being fed from two sources. A HVDC
line connects system A to the load. The HVDC control makes the decision of how
much power is transferred from system A to the load. System B is producing the
power: SB=Sload-SA.
The HVDC model is shown in Figure 12. The valve group system chosen is a six-pulse
converter bridge, monopolar configurations. The valve group is a model from the
master library in PSCAD/EMTDC.

Figure 12 HVDC model.
The HVDC inverter is normally operating in a dc voltage-controlling mode, the constant Us characteristic B-H-E in Figure 6. If the current order increases, the operating point moves towards and beyond point B. Then the inverter mode of control will revert to constant extinction angle control. The DC voltage will be less than the desired value. When the current order is increased to the operating point where the voltage dependent current order limit will meet the minimum extinction angle characteristic, then the maximum power is transferred in the HVDC line. This can be seen in Figure 13. At the start of the simulation the current order is 0.98 [pu], then the dc voltage is at its maximum. When the current order increases we can see that the voltage is starting decreasing. The control system is now controlling at a minimum extinction angle. At the time 1.9 the voltage dependent current order limit is lower than the current order. The maximum point of power transferred in the HVDC line is reached. The voltage will now be constant again at a lower point then it was in the voltage control mode.
The same system is tested for
damping control. Now the HVDC line is in parallel with an AC line. System B is
changed to a synchronous machine with a multimass model. The model can
demonstrate that a HVDC line can damp out oscillations that occur when breakers
opens.

Figure 14 System med HVDC line in parallel
with the AC line.
At 20 seconds part of the load is
disconnected. With no HVDC line, the weak AC line cannot support the load
alone. Also in the simulation in Figure
15, the voltage is too low at the load. However, this
can be justified with more power thru the HVDC line. In Figure 15 the HVDC line have no control of the damping. The
same amount of power is coming out from the HVDC line whatever happens at the
load.

Figure 15 System with HVDC line and no
damping control.
In Figure
16 the same simulation is done as in Figure 15. The difference is damping control has been applied.
It can be seen that the oscillations is smaller in both power and frequency
with damping control.

Figure 16 System with HVDC line and damping
control.
It can also be seen that the power thru the
HVDC line is much less. With damping control the AC line can transfer more
power than with no damping control. At 25 seconds the breakers close again. The
system then returns back to normal.
HVDC offers powerful alternative to increase
stability of a power system as well as to improve system operating flexibility
and loss reduction. Our simulations have shown that HVDC lines can be used for
oscillations’ damping and improvement of the system stability. When a HVDC line
is in parallel with an AC-line, the AC-line can transfer more power because of
the damping control. With damping control the AC line can transfer more power
than with no damping control.
To keep the losses to a minimum, the control
system shall be designed to keep as high voltage as possible. Under steady
state conditions, the inverter is assigned to the task of controlling the dc
voltage. This can be done by maintaining a constant dc voltage. Alternatively,
the inverter may operate at a constant extinction angle g causing the dc voltage to droop with increasing dc current.
If the
inverter is operating in a minimum constant g or constant Ud characteristic, the rectifier must
control the dc current Id.